Rotating electric machine drive system

ABSTRACT

A rotating electric machine drive system includes a rotating electric machine and a drive apparatus. The rotating electric machine includes a Y-connected three-phase stator coil. The drive apparatus supplies electric current to the stator coil and thereby drives the rotating electric machine. In a predetermined high-torque region, the drive apparatus supplies the stator coil with the electric current which has a waveform obtained by superimposing a specific harmonic waveform on a first-order harmonic waveform. The specific harmonic waveform is one of third-order and (3+6n)th-order harmonic waveforms, or a harmonic waveform which is obtained by synthesizing at least two of the third-order and (3+6n)th-order harmonic waveforms, where n is a natural number not less than 1. The specific harmonic waveform takes a negative integral value for a positive half cycle of the first-order harmonic waveform and a positive integral value for a negative half cycle of the first-order harmonic waveform.

CROSS-REFERENCE TO RELATED APPLICATION

This application is based on and claims priority from Japanese PatentApplication No. 2015-218937 filed on Nov. 6, 2015, the content of whichis hereby incorporated by reference in its entirety into thisapplication.

BACKGROUND

1. Technical Field

The present invention relates to rotating electric machine drive systemsthat are used in, for example, motor vehicles to drive electric motorsand electric generators.

2. Description of Related Art

Conventionally, it has been desired for electric motors for electricvehicles to exert high-torque and high-efficiency characteristics over awide operating range from low speed to high speed.

To satisfy such a desire, there has been developed a method of switchingthe connection of a stator coil of an electric motor between a Yconnection (or star connection) and a Δ connection (or delta connection)so as to enable the electric motor to exert optimal characteristics inboth a low-speed region and a high-speed region (see, for example,Japanese Patent Application Publication No. JP2014054094A).

It is required for four-wheel drive vehicles and heavy medium-sized orlarge-sized vehicles to have an excellent hill-climbing ability.Moreover, in an engine-starting operation, diesel engine vehiclesgenerally require twice or more torque than gasoline engine vehicles.

The above-requirements may be met by increasing the amount of electriccurrent supplied to rotating electric machines used in the vehicles orincreasing the sizes of the rotating electric machines.

However, increasing the amount of electric current supplied to therotating electric machines would result in increases in the copper andiron losses of the rotating electric machines. On the other hand,increasing the sizes of the rotating electric machines would make itdifficult for the rotating electric machines to be received in a limitedspace in an engine compartment.

SUMMARY

The inventor of the present application has focused on the third-orderand (3+6n)th-order harmonics which are generally not utilized (orincluded) in the electric current supplied to a stator coil of arotating electric machine since these harmonics may result in anincrease in the iron loss of the rotating electric machine. The inventorhas first found, through research and investigation, that it is possibleto achieve a high efficiency of a rotating electric machine in apredetermined high-torque region by supplying a predetermined harmonicelectric current to a stator coil of the rotating electric machine inthe predetermined high-torque region. The present invention has beenmade based on the above findings by the inventor.

According to the present invention, there is provided a first rotatingelectric machine drive system which includes a rotating electric machineand a drive apparatus. The rotating electric machine includes aY-connected three-phase stator coil and a rotor that produces bothmagnet torque and reluctance torque. The drive apparatus supplieselectric current to the stator coil and thereby drives the rotatingelectric machine. In a predetermined high-torque region, the driveapparatus supplies the stator coil with the electric current which has awaveform obtained by superimposing a specific harmonic waveform on afirst-order harmonic waveform. The specific harmonic waveform is one ofthird-order and (3+6n)th-order harmonic waveforms, or a harmonicwaveform which is obtained by synthesizing at least two of thethird-order and (3+6n)th-order harmonic waveforms, where n is a naturalnumber greater than or equal to 1. The specific harmonic waveform takesa negative integral value for a positive half cycle of the first-orderharmonic waveform and a positive integral value for a negative halfcycle of the first-order harmonic waveform.

In the rotating electric machine having the rotor producing both themagnet torque and the reluctance torque, the magnet torque isproportional to Ψ×Iq and the reluctance torque is proportional to(Lq−Ld)×Id×Iq, where is magnet magnetic flux, Iq is q-axis electriccurrent, Id is d-axis electric current, Lq is q-axis inductance and Ldis d-axis inductance.

In general, in using the reluctance torque, the magnetic force ofmagnets is weakened, causing a loss. Therefore, in a low-torque regionwhere the electric current is low, it is efficient to use Ψ×Iq ratherthan (Lq−Ld)×Id×Iq. Moreover, in the case where the magnets areimplemented by strong magnets (e.g., sintered neodymium magnets), thetotal torque is higher when the magnet torque is used than when thereluctance torque is used. Accordingly, in the low-torque region, it ispreferable to increase the magnet magnetic flux Ψ and the q-axiselectric current Iq.

On the other hand, when the electric current is high, the reluctancetorque is higher than the magnet torque even in a state where the magnetmagnetic flux is high. This is because the reluctance torque is aquadratic function of the electric current (i.e., proportional toId×Iq), whereas the magnet torque is a linear function of the electriccurrent (i.e., proportional to Iq). Accordingly, in this case, it ispreferable to increase the reluctance torque by increasing (Lq−Ld).Further, to increase (Lq−Ld), it is preferable to increase the q-axisinductance Lq while reducing the magnet magnetic flux Ψ and the d-axisinductance Ld by increasing the d-axis magnetic reluctance.

In the first rotating electric machine drive system according to thepresent invention, in the predetermined high-torque region, the driveapparatus supplies the stator coil with the electric current which hasthe waveform obtained by superimposing the specific harmonic waveform onthe first-order harmonic waveform. Consequently, it is possible toincrease the q-axis inductance Lq; it is also possible to increase thed-axis magnetic reluctance, thereby reducing the magnet magnetic flux Ψand the d-axis inductance Ld. As a result, it is possible to increasethe total torque produced by the rotor, thereby achieving a highefficiency of the rotating electric machine in the predeterminedhigh-torque region.

According to the present invention, there is also provided a secondrotating electric machine drive system which includes a rotatingelectric machine and a drive apparatus. The rotating electric machineincludes a stator and a rotor. The stator includes a stator core and athree-phase stator coil mounted on the stator core. The stator coil isconfigured to be switchable between a Y connection and a Δ connection.The rotor is configured to produce both magnet torque and reluctancetorque. The drive apparatus supplies electric current to the stator coiland thereby drives the rotating electric machine. In a predeterminedhigh-torque region where the magnet torque produced by the rotor islower than the reluctance torque produced by the rotor, the driveapparatus supplies the electric current to the stator coil with thestator coil switched to the Δ connection.

With the above configuration, in the predetermined high-torque region,it is possible for the drive apparatus to supply the Δ-connected statorcoil with the electric current which has a waveform obtained bysuperimposing a specific harmonic waveform on a first-order harmonicwaveform. The specific harmonic waveform is one of the third-order and(3+6n)th-order harmonic waveforms or a harmonic waveform which isobtained by synthesizing at least two of the third-order and(3+6n)th-order harmonic waveforms, where n is a natural number greaterthan or equal to 1. The specific harmonic waveform takes a negativeintegral value for a positive half cycle of the first-order harmonicwaveform and a positive integral value for a negative half cycle of thefirst-order harmonic waveform. Consequently, it is possible to increasethe q-axis inductance Lq; it is also possible to increase the d-axismagnetic reluctance, thereby reducing the magnet magnetic flux Ψ and thed-axis inductance Ld. As a result, it is possible to increase the totaltorque produced by the rotor, thereby achieving a high efficiency of therotating electric machine in the predetermined high-torque region.

In addition, the lower the frequency of the specific harmonic waveformused in the above first and second rotating electric machine drivesystems, the higher the amplitude of the specific harmonic waveform.Therefore, to more reliably achieve the above-described advantageouseffects, it is preferable to set the frequency of the specific harmonicwaveform as low as possible.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will be understood more fully from the detaileddescription given hereinafter and from the accompanying drawings ofexemplary embodiments, which, however, should not be taken to limit theinvention to the specific embodiments but are for the purpose ofexplanation and understanding only.

In the accompanying drawings:

FIG. 1 is a schematic configuration diagram of a rotating electricmachine drive system according to a first embodiment;

FIG. 2 is a schematic view, along an axial direction, of part of arotating electric machine included in the rotating electric machinedrive system;

FIG. 3 is a schematic circuit diagram of the rotating electric machinedrive system;

FIG. 4 is a waveform chart illustrating electric current supplied to astator coil of a stator of the rotating electric machine in the rotatingelectric machine drive system;

FIG. 5 is a schematic view illustrating both the flow of magnetic fluxalong a d-axis magnetic flux path and the flow of magnetic flux along aq-axis magnetic flux path in the rotating electric machine;

FIG. 6 is a schematic view illustrating magnetic flux in the stator whenthe electric current having a specific harmonic waveform is supplied tothe stator coil;

FIG. 7 is a graphical representation illustrating the magnet torque,reluctance torque and total torque of an Interior Permanent Magnet (IPM)motor in a power running control region;

FIG. 8 is a graphical representation illustrating the magnet torque,reluctance torque and total torque of the IPM motor in a regenerativebraking control region;

FIG. 9 is a graphical representation illustrating the relationshipbetween the rotational speed and torque of the rotating electric machineaccording to the first embodiment both when the stator coil isΔ-connected and when the stator coil is Y-connected;

FIG. 10 is a schematic circuit diagram of a rotating electric machinedrive system according to a second embodiment;

FIG. 11 is a schematic view, along an axial direction, of part of arotating electric machine included in a rotating electric machine drivesystem according to a third embodiment;

FIG. 12 is an enlarged view of a region A of FIG. 11;

FIG. 13 is a schematic view illustrating the distribution of magneticflux density on a radially outer surface of part of a rotor of therotating electric machine according to the third embodiment, the part ofthe rotor corresponding to one magnetic pole of the rotor;

FIG. 14 is a schematic view illustrating the part of the rotorcorresponding to one magnetic pole and stator teeth through whichmagnetic flux effective for a U-phase winding of a stator coil passes;

FIG. 15 is a schematic view illustrating the part of the rotorcorresponding to one magnetic pole and one of the stator teeth throughwhich the magnetic flux effective for the U-phase winging passes;

FIG. 16 is a schematic view illustrating the distribution of magneticflux density on the radially outer surface of the part of the rotorcorresponding to one magnetic pole;

FIG. 17 is a schematic view illustrating the magnetic flux through thestator tooth shown in FIG. 15 when the stator tooth passes by theradially outer surface of the part of the rotor corresponding to onemagnetic pole;

FIG. 18 is a schematic view illustrating the magnetic flux crossing theU-phase winding, which is equal to the sum of the magnetic fluxesrespectively through the five unshaded stator teeth in FIG. 14;

FIG. 19 is a schematic view illustrating the density of magnetic fluxwhich passes through each stator tooth when the stator tooth passes bythe radially outer surface of the part of the rotor corresponding to onemagnetic pole;

FIG. 20 is a graphical representation illustrating a third-orderharmonic when an arc ratio θa of each magnetic pole of the rotor is setto 120° in electrical angle;

FIG. 21 is a schematic view illustrating the reason of setting the arcratio θa to be greater than 120° in electrical angle in the thirdembodiment;

FIG. 22 is another schematic view illustrating the reason of setting thearc ratio θa to be greater than 120° in electrical angle in the thirdembodiment;

FIG. 23 is a schematic circuit diagram of the rotating electric machinedrive system according to the third embodiment;

FIG. 24 is a schematic view illustrating the arc ratio θa of eachmagnetic pole of a rotor according to a first modification of the thirdembodiment;

FIG. 25 is an enlarged view of a region B of FIG. 24;

FIG. 26 is a schematic view illustrating the arc ratio θa of eachmagnetic pole of a rotor according to a second modification of the thirdembodiment;

FIG. 27 is a schematic view illustrating the arc ratio θa of eachmagnetic pole of a rotor according to a third modification of the thirdembodiment;

FIG. 28 is a schematic view, along an axial direction, of part of arotating electric machine included in a rotating electric machine drivesystem according to a fourth embodiment;

FIG. 29 is a schematic view illustrating one magnetic pole of a rotorand stator teeth receiving magnetic flux from the magnetic pole of therotor in the rotating electric machine according to the fourthembodiment;

FIG. 30 is a schematic view illustrating an electrical angular rangewithin which the stator teeth receive magnetic flux from the magneticpole of the rotor;

FIG. 31 is a schematic view, along an axial direction, of part of arotating electric machine included in a rotating electric machine drivesystem according to a fifth embodiment; and

FIG. 32 is a schematic view, along an axial direction, of part of arotor according to a comparative example.

DESCRIPTION OF EMBODIMENTS

Exemplary embodiments will be described hereinafter with reference toFIGS. 1-32. It should be noted that for the sake of clarity andunderstanding, identical components having identical functionsthroughout the whole description have been marked, where possible, withthe same reference numerals in each of the figures and that for the sakeof avoiding redundancy, descriptions of identical components will not berepeated.

First Embodiment

FIG. 1 shows the overall configuration of a rotating electric machinedrive system according to the first embodiment. The rotating electricmachine drive system includes a rotating electric machine 1, an inverter40 that functions as a drive apparatus to drive the rotating electricmachine 1, and an electric power source B.

In the present embodiment, the rotating electric machine 1 is configuredas an electric motor for use in a motor vehicle.

As shown in FIG. 1, the rotating electric machine 1 includes a housing10, a rotating shaft 13, a rotor 20 and a stator 30.

The housing 10 has a hollow cylindrical shape with both axial endsclosed. The housing 10 is comprised of a pair of cup-shaped housingpieces 10 a and 10 b which are fixed together at the open ends thereofby, for example, a plurality of bolts 11.

The rotating shaft 13 is rotatably supported by the housing 10 via apair of bearings 12 that are provided respectively in opposite axial endwalls of the housing 10.

The rotor 20 is received in the housing 10 and fixedly fitted on anaxially central part of the rotating shaft 13 so as to rotate togetherwith the rotating shaft 13. The rotor 20 functions as a field to produceboth magnet torque and reluctance torque.

As shown in FIG. 2, the rotor 20 includes a rotor core 21 and aplurality of permanent magnets 23 embedded in the rotor core 21. That isto say, in the present embodiment, the rotor 20 is configured as anInterior Permanent Magnet (IPM) rotor.

The rotor core 21 is formed, by axially laminating a plurality ofannular magnetic steel sheets, into a hollow cylindrical shape.Consequently, at the radial center of the rotor core 21, there is formeda through-hole 21 a, in which the rotating shaft 13 is fixedly fitted soas to rotate together with the rotor core 21.

The permanent magnets 23 are embedded in the rotor core 21 so as to forma plurality of magnetic poles of the rotor 20 on the radially outerperiphery of the rotor core 21. The magnetic poles are equally spaced inthe circumferential direction of the rotor core 21 at predeterminedintervals so that the polarities of the magnetic poles alternate betweenN (North) and S (South) in the circumferential direction. In addition,in the present embodiment, the number of the magnetic poles of the rotor20 is equal to, for example, 8 (i.e., 4 N poles and 4 S poles).

More specifically, in the present embodiment, the rotor core 21 has aplurality (e.g., eight) of pairs of magnet-receiving holes 22 formed inthe vicinity of the radially outer periphery of the rotor core 21. Eachof the magnet-receiving holes 22 extends in the axial direction of therotor core 21 so as to penetrate the rotor core 21 in the axialdirection. Further, each of the magnet-receiving holes 22 has asubstantially rectangular cross section perpendicular to a longitudinalaxis O of the rotor core 21 (or the axis of rotation of the rotor 20).

In addition, it should be noted that though there is shown only one pairof the magnet-receiving holes 22 in FIG. 2, the plurality of pairs ofthe magnet-receiving holes 22 are equally spaced in the circumferentialdirection of the rotor core 21 at predetermined intervals.

Moreover, in the present embodiment, each pair of the magnet-receivingholes 22 is arranged so as to form a substantially V-shape that openstoward the radially outer periphery of the rotor core 21. Further, foreach pair of the magnet-receiving holes 22, there is formed acorresponding center bridge 24 of the rotor core 21 which extends in aradial direction of the rotor core 21 at a substantially constant widthso as to separate the two magnet-receiving holes 22 of the pair fromeach other. The corresponding center bridge 24 is provided for causingmagnetic flux saturation and thereby impeding formation of a magneticcircuit between the two magnet-receiving holes 22.

Each of the permanent magnets 23 is inserted in a corresponding one ofthe magnet-receiving holes 22 of the rotor core 21 so as to extend inthe axial direction of the rotor core 21. Further, each of the permanentmagnets 23 has a substantially rectangular cross section perpendicularto the axial direction of the rotor core 21 (i.e., the direction of thelongitudinal axis O of the rotor core 21). That is to say, in thepresent embodiment, each of the permanent magnets 23 has a substantiallycuboid shape.

Moreover, for each pair of the magnet-receiving holes 22 of the rotorcore 21, the two permanent magnets 23 which are respectively inserted inthe two magnet-receiving holes 22 of the pair are arranged so that thepolarities (N or S) of the two permanent magnets 23 are the same on theradially outer periphery of the rotor core 21. Consequently, the twopermanent magnets 23 together form one of the magnetic poles of therotor 20 on the radially outer periphery of the rotor core 21. Inaddition, as shown in FIG. 2, when viewed along the axial direction ofthe rotor core 21, the two permanent magnets 23 are symmetricallyarranged and extend obliquely with respect to a centerline C1 of themagnetic pole; the centerline C1 extends in the radial direction, alongwhich the corresponding center bridge 24 of the rotor core 21 is formed,and bisects the magnetic pole in the circumferential direction of therotor core 21. Consequently, the two permanent magnets 23 also togetherform a substantially V-shape that opens radially outward (i.e., towardthe radially outer periphery of the rotor core 21).

The rotor core 21 also has a plurality of q-axis core portions 27through which q-axis magnetic flux flows. Each of the q-axis coreportions 27 is formed between a corresponding circumferentially-adjacentpair of the magnetic poles of the rotor 20. Further, for each of themagnet-receiving holes 22 of the rotor core 21, there is provided afirst magnetic flux barrier (or magnetic void) 25 between thecorresponding permanent magnet 23 received in the magnet-receiving hole22 and the corresponding q-axis core portion 27 adjacent to themagnet-receiving hole 22. In other words, the first magnetic fluxbarrier 25 is provided on the corresponding q-axis core portion 27 sideof the magnet-receiving hole 22.

Moreover, for each pair of the magnet-receiving holes 22 of the rotorcore 21, there are provided a pair of second magnetic flux barriers 26that respectively extend from centerline C1-side ends of the pair of themagnet-receiving holes 22 toward the longitudinal axis O of the rotorcore 21. Further, the corresponding center bridge 24, which is formedbetween the pair of the magnet-receiving holes 22, is radially extendedtoward the longitudinal axis O of the rotor core 21 so as to alsoseparate the pair of the second magnetic flux barriers 26 from eachother.

In addition, in the present embodiment, each of the first and secondmagnetic flux barriers 25 and 26 is provided in the form of an air gapin the rotor core 21.

Referring to FIGS. 1 and 2, the stator 30 includes a hollow cylindrical(or annular) stator core 31 and a three-phase stator coil 35 mounted onthe stator core 31.

The stator core 31 is disposed radially outside the rotor 20 so that theradially inner surface of the stator core 31 faces the radially outersurface of the rotor core 21 through a predetermined air gap formedtherebetween. The stator core 31 is fixed to the inner circumferentialsurface of the housing 10. More specifically, the stator core 31 isaxially fixedly sandwiched between the pair of housing pieces 10 a and10 b (see FIG. 1).

In the present embodiment, the stator core 31 is formed by axiallylaminating a plurality of magnetic steel sheets into the hollowcylindrical shape.

The stator core 31 includes an annular back core portion 32, a pluralityof teeth 33 and a plurality of slots 34. The teeth 33 each extendradially inward from the back core portion 32 and are spaced from oneanother at a predetermined pitch in the circumferential direction of thestator core 31 (or the circumferential direction of the back coreportion 32). Each of the slots 34 is formed between onecircumferentially-facing pair of side surfaces of the teeth 33 so as toradially extend to open on the radially inner surface of the stator core31. In addition, each of the teeth 33 has a pair of protrusions 33 aformed at a distal end (or radially inner end) thereof so as to protruderespectively toward opposite circumferential sides.

In the present embodiment, the number of the slots 34 formed permagnetic pole of the rotor 20 that has the eight magnetic poles and perphase of the three-phase stator coil 35, namely, the slot multipliernumber is equal to 2. Accordingly, the total number Sn of the slots 34formed in the stator core 31 can be determined by the followingequation: Sn=S×Mn×P=2×8×3=48, where S is the slot multiplier number, Mnis the number of the magnetic poles of the rotor 20 and P is the numberof phases of the stator coil 35.

The stator coil 35 is mounted on the stator core 31 so as to be receivedin the slots 34 of the stator core 31.

As shown in FIG. 3, in the present embodiment, the stator coil 35includes a U-phase winding, a V-phase winding and a W-phase winding thatare Y-connected to define a neutral point therebetween. Morespecifically, each of the U-phase, V-phase and W-phase windings hasfirst and second ends. The first ends of the U-phase, V-phase andW-phase windings are connected with each other at the neutral point. Thesecond ends of the U-phase, V-phase and W-phase windings are connectedrespectively with output terminals U1, V1 and W1 of the inverter 40.

The inverter 40 includes three upper arm units 41 and three lower armunits 41. Each of the upper and lower arm units 41 includes an IGBT(Insulated Gate Bipolar Transistor) 41 a and a flyback diode (orfreewheeling diode) 41 b that are connected in parallel with each other.The inverter 40 also includes a smoothing capacitor 42 that smoothesalternating current on the electric power source B side.

The inverter 40 has the same functions as a well-known PWM controlinverter. Based on a PWM (Pulse Width Modulation) signal which is acontrol output signal for a V/F control or a vector control, the IGBTs41 a of the upper and lower arm units 41 are repeatedly turned on andoff, thereby generating three-phase AC voltage. More specifically, theIGBTs 41 a of the upper arm units 41 are operated in inverse relation tothe IGBTs 41 a of the lower arm units 41; thus the IGBTs 41 a of theupper arm units 41 are not turned on at the same time as the IGBTs 41 aof the lower arm units 41. In addition, the on/off operations of theIGBTs 41 a of the upper and lower arm units 41 are controlled by anot-shown ECU (Electronic Control Unit) based on a signal outputted froma not-shown position sensor that senses the rotational position of therotor 20 of the rotating electric machine 1.

In the present embodiment, in a predetermined high-torque region, theinverter 40 supplies the stator coil 35 with electric current (orcontrol current) having a waveform as shown with a one-dot chain line inFIG. 4. The waveform is obtained by superimposing a specific harmonicwaveform as shown with a continuous line in FIG. 4 on a first-orderharmonic waveform as shown with a dashed line in FIG. 4. The first-orderharmonic waveform is a fundamental control waveform. The specificharmonic waveform is one of third-order and (3+6n)th-order harmonicwaveforms, or a harmonic waveform which is obtained by synthesizing atleast two of the third-order and (3+6n)th-order harmonic waveforms,where n is a natural number greater than or equal to 1. The specificharmonic waveform takes a negative integral value for a positive halfcycle of the first-order harmonic waveform (e.g., the half cycle from 0°to 180° in FIG. 4) and a positive integral value for a negative halfcycle of the first-order harmonic waveform (e.g., the half cycle from180° to 360° in FIG. 4). In other words, the integral value of thespecific harmonic waveform for a positive half cycle of the first-orderharmonic waveform is negative; the integral value of the specificharmonic waveform for a negative half cycle of the first-order harmonicwaveform is positive. More particularly, in the present embodiment, thespecific harmonic waveform is the third-order harmonic waveform as shownin FIG. 4. Consequently, by supplying the above electric current to thestator coil 35, it is possible to increase the q-axis inductance Lq,thereby increasing the reluctance torque and thus the total torqueproduced by the rotor 20. In addition, the third-order and(3+6n)th-order harmonics may be together referred to as harmonics of thethird-order group.

Next, the principle of increasing the reluctance torque using theharmonics of the third-order group according to the present embodimentwill be described.

In FIG. 5, a d-axis magnetic flux path is shown with a continuous line,and a q-axis magnetic flux path is shown with a dashed line. Along thed-axis magnetic flux path, d-axis magnetic flux flows between the rotor20 and the stator 30. Along the q-axis magnetic flux path, q-axismagnetic flux flows between the rotor 20 and the stator 30. Moreover, inFIG. 5, the continuous-line arrows indicate stator magnetic flux whichis generated in the stator 30 when electric current having thefirst-order harmonic waveform is supplied to the stator coil 35. Thelonger the continuous-line arrows, the higher the strength of the statormagnetic flux.

On the other hand, in FIG. 6, the continuous-line arrows indicate statormagnetic flux which is generated in the stator 30 when electric currenthaving the specific harmonic waveform is supplied to the stator coil 35.In the present embodiment, each phase winding of the stator coil 35 isarranged in a plurality of pairs of circumferentially adjacent slots 34of the stator core 31. As seen from FIG. 6, for each of the pairs ofcircumferentially adjacent slots 34, the stator magnetic flux flows inopposite radial directions respectively on opposite circumferentialsides of the pair of circumferentially adjacent slots 34.

Moreover, as seen from FIGS. 5 and 6, along the q-axis magnetic fluxpath, the stator magnetic flux generated by the electric current havingthe first-order harmonic waveform and the stator magnetic flux generatedby the electric current having the specific harmonic waveform flow inthe same radial direction and thus are strengthened by each other (oradded to each other). Consequently, the magnetic reluctance along thed-axis magnetic flux path is increased, making it difficult for magneticflux to flow along the d-axis magnetic flux path. As a result, bysupplying the stator coil 35 with the electric current having thewaveform obtained by superimposing the specific harmonic waveform on thefirst-order harmonic waveform, it becomes possible to increase thereluctance torque.

In the present embodiment, the high-torque region is predetermined as anoperating region of the rotating electric machine 1 where the magnettorque produced by the rotor 20 is lower than the reluctance torqueproduced by the rotor 20.

Hereinafter, the high-torque region will be described in more detail bytaking an IPM motor, where the ratio between the maximum values (oramplitudes) of the magnet torque and reluctance torque is 1:1, as anexample.

FIG. 7 illustrates the magnet torque, reluctance torque and total torqueof the IPM motor in a power running control region. On the other hand,FIG. 8 illustrates the magnet torque, reluctance torque and total torqueof the IPM motor in a regenerative braking control region.

As shown in FIG. 7, in the power running control region, where thecontrol advance angle is in the range of 90° to 180°, the magnet torqueand the reluctance torque become equal to each other when the controladvance angle is equal to 120°. Moreover, the magnet torque is lowerthan the reluctance torque when the control advance angle is greaterthan 120° and less than or equal to 180°. In addition, when the controladvance angle is in the range of 120° to 180°, a Y connection is moreadvantageous than a Δ connection.

As shown in FIG. 8, in the regenerative braking control region, wherethe control advance angle is in the range of 180° to 270°, the magnettorque and the reluctance torque become equal to each other when thecontrol advance angle is equal to 240°. Moreover, the magnet torque islower than the reluctance torque when the control advance angle isgreater than or equal to 180° and less than 240°. In addition, when thecontrol advance angle is in the range of 180° to 240°, a Y connection ismore advantageous than a Δ connection.

It should be noted that the above ranges of 120° to 180° and 180° to240° may be varied according to the ratio between the maximum values ofthe magnet torque and reluctance torque.

Moreover, in the present embodiment, the high-torque region ispredetermined so that in the high-torque region, the following Equation(1) is satisfied:

T=pΨIq+p(Lq−Ld)IdIq  (1)

where T is the total torque produced by the rotor 20, p is the number ofmagnetic pole pairs of the rotor 20, T is the magnet magnetic flux, Iqis the q-axis electric current, Id is the d-axis electric current, Lq isthe q-axis inductance and Ld is the d-axis inductance.

According to the present embodiment, it is possible to achieve thefollowing advantageous effects.

In the present embodiment, the rotating electric machine drive systemincludes the rotating electric machine 1 and the inverter (or driveapparatus) 40. The rotating electric machine 1 includes the Y-connectedthree-phase stator coil 35 and the rotor 20 that produces both themagnet torque and the reluctance torque. The inverter 40 drives therotating electric machine 1. In the predetermined high-torque region,the inverter 40 supplies the stator coil 35 with the electric currentwhich has the waveform obtained by superimposing the specific harmonicwaveform on the first-order harmonic waveform. The specific harmonicwaveform is one of the third-order and (3+6n)th-order harmonic waveformsor a harmonic waveform which is obtained by synthesizing at least two ofthe third-order and (3+6n)th-order harmonic waveforms, where n is anatural number greater than or equal to 1. The specific harmonicwaveform takes a negative integral value for a positive half cycle ofthe first-order harmonic waveform and a positive integral value for anegative half cycle of the first-order harmonic waveform.

With the above configuration, in the predetermined high-torque region,by supplying the stator coil 35 with the electric current having thewaveform obtained by superimposing the specific harmonic waveform on thefirst-order harmonic waveform, it is possible to increase the q-axisinductance Lq, thereby increasing the reluctance torque. Consequently,it is possible to increase the total torque produced by the rotor 20,thereby achieving a high efficiency of the rotating electric machine 1in the predetermined high-torque region as shown in FIG. 9.

In the present embodiment, the high-torque region is predetermined as anoperating region of the rotating electric machine 1 where the magnettorque produced by the rotor 20 is lower than the reluctance torqueproduced by the rotor 20.

Predetermining (or setting) the high-torque region as above, it ispossible to reliably achieve a high efficiency of the rotating electricmachine 1 in the high-torque region.

In the present embodiment, the high-torque region is predetermined sothat in the high-torque region, the above Equation (1) is satisfied.

Accordingly, it is possible to easily predetermine (or set) thehigh-torque region based on the above Equation (1).

Second Embodiment

A rotating electric machine drive system according to the secondembodiment has a similar configuration to the rotating electric machinedrive system according to the first embodiment. Therefore, thedifferences therebetween will be mainly described hereinafter.

As shown in FIG. 10, in the present embodiment, the U-phase, V-phase andW-phase windings of the stator coil 35 of the rotating electric machine1 are Δ-connected, instead of being Y-connected as in the firstembodiment. Therefore, it is impossible to expect an increase ofefficiency in an operating region of the rotating electric machine 1where the reluctance torque is higher than the magnet torque.

However, depending on the characteristics of the inverter (or driveapparatus) 40, it is possible to achieve more advantages in comparisonwith the combination of an ordinary (or general-purpose) inverter and aΔ connection.

In the case of consumer products, more particularly those consumerproducts which are operated in the vicinities of the users, the PWMfrequencies of motor drivers are mostly set above the audible range (oraudio-frequency range), i.e., set to be higher than 20 kHz, so as toimprove the degree of satisfaction of the users.

On the other hand, in the PWM control of existing inverters used inmotor vehicles, the PWM frequencies are mostly set to be not higher thanthe audible range, more particularly to be in the range of 8 to 12 kHz,so as to secure the system robustness. Moreover, in a high-electriccurrent region, the PWM frequencies are generally set to be not higherthan half the respective maximum values, thereby supplying high electriccurrent with less switching losses of the inverters. In these cases, itis easy for sine waves produced by the PWM control to contain thewaveforms of third-order and 3(6n−1)th-order harmonics caused byexciting current of the inverters. Furthermore, in the case ofperforming an overmodulation control for extending the region of use,sine waves are no longer produced, so as to increase the voltage appliedto the motor terminals; in this case, the waveform of electric currentoutputted from the inverters still contains the waveforms of third-orderand 3(6n−1)th-order harmonics.

Moreover, in most cases, stator coils of rotating electric machines usedin motor vehicles are designed to have a resistance in the order of mΩ,so as to suppress heat produced by the stator coils. Thus, the statorcoils have a small number of turns and low impedance. Therefore, in thecase of the stator coils being Δ-connected, electric current isgenerally supplied to the stator coils to cancel circulating currentthat circulates in the Δ connection; the electric current is inverse inphase and identical in amplitude to the third-order and 3(6n−1)th-orderharmonics of the circulating current.

In comparison, in the present embodiment, in the predeterminedhigh-torque region where the magnet torque produced by the rotor 20 islower than the reluctance torque produced by the rotor 20, the inverter40 performs either a PWM control with the PWM frequency being not higherthan the audible range (more specifically, being in the range of 8 to 20kHz) or an overmodulation control. Moreover, by configuring the rotatingelectric machine 1 as to be described in the following third and fourthembodiments, it is possible to utilize the third-order and3(6n−1)th-order harmonics of the circulating current that circulates inthe Δ-connected stator coil 35. Consequently, it is possible to increase(Lq−Ld), thereby increasing the reluctance torque and thus the totaltorque produced by the rotor 20 in the predetermined high-torque region.

Third Embodiment

A rotating electric machine drive system according to the thirdembodiment has a similar configuration to the rotating electric machinedrive system according to the first embodiment. Therefore, thedifferences therebetween will be mainly described hereinafter.

In the first embodiment, the stator coil 35 of the rotating electricmachine 1 is Y-connected. Moreover, the electric current supplied fromthe inverter (or drive apparatus) 40 to the stator coil 35 is controlledso as to achieve a high efficiency of the rotating electric machine 1.

In comparison, in the present embodiment, the stator coil 35 of therotating electric machine 1 is configured to be switchable between a Yconnection and a Δ connection. A drive apparatus 50 is provided, insteadof the inverter 40 described in the first embodiment, to drive therotating electric machine 1. In the predetermined high-torque region,the drive apparatus 50 supplies electric current to the stator coil 35with the stator coil 35 switched to the Δ connection. Moreover, insteadof controlling the electric current supplied from the drive apparatus 50to the stator coil 35, an arc ratio θa of each magnetic pole of therotor 20 is set so as to create the specific harmonic waveform describedin the first embodiment, thereby achieving a high efficiency of therotating electric machine 1.

As shown in FIG. 11, in the present embodiment, none of the teeth 33 ofthe stator core 31 have protrusions 33 a formed at a distal end (orradially inner end) thereof, unlike in the first embodiment. That is, inthe present embodiment, each of the teeth 33 radially extends straightwithout circumferentially protruding at the distal end thereof.

In the present embodiment, the rotor 20 includes eight pairs ofpermanent magnets 23, as in the first embodiment. The eight pairs ofpermanent magnets 23 form eight magnetic poles (i.e., 4 N poles and 4 Spoles) on the radially outer periphery of the rotor core 21 so that thepolarities of the magnetic poles alternate between N and S in thecircumferential direction. Moreover, the arc ratio (or angular range) θaof each magnetic pole of the rotor 20 is set to be greater than 120° inelectrical angle, so as to create the specific harmonic waveform.

In addition, as described in the first embodiment, the specific harmonicwaveform is one of the third-order and (3+6n)th-order harmonic waveformsor a harmonic waveform which is obtained by synthesizing at least two ofthe third-order and (3+6n)th-order harmonic waveforms, where n is anatural number greater than or equal to 1. The specific harmonicwaveform takes a negative integral value for a positive half cycle ofthe first-order harmonic waveform and a positive integral value for anegative half cycle of the first-order harmonic waveform.

In the present embodiment, for each magnetic pole of the rotor 20, thearc ratio θa represents the angular range within which magnetic fluxradially flows from the pair of permanent magnets 23 forming themagnetic pole to the stator 30.

More specifically, in the present embodiment, as shown in FIGS. 11 and12, the arc ratio θa is defined as an angle between first and secondimaginary lines L1 and L2. The first imaginary line L1 extends straightthrough both the longitudinal axis O of the rotor core 21 (or the axisof rotation of the rotor 20) and an intersection point P1; theintersection point P1 is formed between an extension wall surface 22 a,which extends from a radially outer wall surface of the magnet-receivinghole 22 of the rotor core 21 receiving one of the pair of permanentmagnets 23 (i.e., the left-side permanent magnet 23 in FIG. 11) towardthe first magnetic flux barrier 25 adjacent to the magnet-receiving hole22, and a radially inner wall surface 28 a of acircumferentially-extending bridge 28 of the rotor core 21 which definesthe first magnetic flux barrier 25. On the other hand, the secondimaginary line L2 extends straight through both the longitudinal axis Oof the rotor core 21 and an intersection point P2; the intersectionpoint P2 is formed between an extension wall surface 22 a, which extendsfrom a radially outer wall surface of the magnet-receiving hole 22 ofthe rotor core 21 receiving the other of the pair of permanent magnets23 (i.e., the right-side permanent magnet 23 in FIG. 11) toward thefirst magnetic flux barrier 25 adjacent to the magnet-receiving hole 22,and a radially inner wall surface 28 a of a circumferentially-extendingbridge 28 of the rotor core 21 which defines the first magnetic fluxbarrier 25.

Next, the reason of setting the arc ratio θa to be greater than 120° inelectrical angle will be described with reference to FIGS. 13-22.

As shown in FIG. 13, magnetic flux flowing from the permanent magnets 23to the radially outer surface of the rotor 20 (i.e., the radially outersurface of the rotor core 21) is oriented so as to be evenly emitted tothe air gap formed between the rotor 20 and the stator 30.

In addition, in most cases, the waveform of magnetic flux density asshown in FIG. 13 is inclined (or slanted) at the circumferential ends ofeach magnetic pole of the rotor 20 due to the difference of magneticreluctance caused by the circumferentially-extending bridges 28 androunded corners of the pair of permanent magnets 23 forming the magneticpole; the circumferentially-extending bridges 28 are respectively formedon opposite circumferential sides of the pair of permanent magnets 23forming the magnetic pole to cause magnetic flux saturation.

Referring now to FIG. 14, magnetic flux generated in the rotatingelectric machine 1 will be explained by taking the U-phase winding ofthe stator coil 35 as an example. In addition, in the presentembodiment, the stator coil 35 is mounted on the stator core 31 in adistributed winding manner with the slot multiplier number set to 2.

The magnetic flux which is effective for the U-phase winding passesthrough all the teeth 33 of the stator core 31 shown in FIG. 14 exceptfor the shaded tooth (i.e., the leftmost tooth) 33.

Moreover, for explaining the magnetic flux crossing the U-phase winding,the magnetic flux passing through one of the unshaded teeth 33 of thestator core 31 will be first explained with reference to FIGS. 15-17.

During rotation of the rotor 20, the tooth 33 of the stator core 31shown in FIG. 15 passes by the radially outer surface of that part ofthe rotor 20 which corresponds to one magnetic pole of the rotor 20. Thedistribution of magnetic flux density on the radially outer surface ofthe part of the rotor 20 is as shown in FIG. 16. When the tooth 33 ofthe stator core 31 passes by the radially outer surface of the part ofthe rotor 20, the magnetic reluctance between the tooth 33 and the partof the rotor 20 is lowered and thus leakage magnetic flux, which hasbeen leaked to the circumferentially-extending bridges 28 and the airgap between the rotor 20 and the stator 30 due to the difference ofmagnetic reluctance, comes to flow to the tooth 33. Consequently, thewaveform of the magnetic flux through the tooth 33 of the stator core 31with respect to the advancing angle of the tooth 33 has a basicallyrectangular shape as shown in FIG. 17.

Moreover, the magnetic flux crossing the U-phase winding is equal to thesum of the magnetic fluxes respectively through the five unshaded teeth33 of the stator core 31 in FIG. 14, and thus equal to the sum ofmagnetic fluxes respectively generated in the five slots 34 of thestator core 31 which are circumferentially offset from one another by30° in electrical angle. As shown in FIG. 18, the waveform of themagnetic flux crossing the U-phase winding contains the 11th-order and13th-order harmonic waveforms and thus has rectangularity occurringtherein. In addition, it is well-known that the 5+6(n−1)th-orderharmonic is generated in a rotating electric machine where the slotmultiplier number is equal to n.

Moreover, voltages (or counterelectromotive forces) Eu, Ev and Ew, whichare respectively generated by the magnetic fluxes crossing the U-phase,V-phase and W-phase windings of the stator coil 35, have symmetry andthus can be expressed by the following equations:

Eu=Em ₁ sin(ωt−0°)+Em ₃ sin 3ωt+Em ₅ sin(5ωt−0°)+ . . . ;

Ev=Em ₁ sin(ωt−120°)+Em ₃ sin 3ωt+Em ₅ sin(5ωt−240°)+ . . . ;

and

Ew=Em ₁ sin(ωt−240°)+Em ₃ sin 3ωt+Em ₅ sin(5ωt−120°)+ . . . ,

where Em₁ is the amplitude of the first-order harmonic, Em₃ is theamplitude of the third-order harmonic, Em₅ is the amplitude of thefifth-order harmonic, ω is the angular velocity and t is time.

In the present embodiment, Em₃ sin 3ωt is utilized which is in the samephase for all of Eu, Ev and Ew. Therefore, it is necessary to generateEm₃ sin 3ωt.

Furthermore, as shown in FIG. 19, the rectangular waveform of thedensity of magnetic flux through each tooth 33 of the stator core 31also has symmetry and can be expressed by the following equation:

Bt=Am ₁ sin ωt+Am ₃ sin 3ωt+Am ₅ sin(5ωt−a)+Am ₇ sin(7ωt−b)+ . . . ,

where Bt is the density of magnetic flux which changes with time t, Am₁is the amplitude of the first-order harmonic, Am₃ is the amplitude ofthe third-order harmonic, Am₅ is the amplitude of the fifth-orderharmonic, Am₇ is the amplitude of the seventh-order harmonic, ω is theangular velocity and a and b are phase shifts.

When the arc ratio θa is equal to 120° in electrical angle, therectangular waveform contains no waveforms of the harmonics of thethird-order group. That is, when the arc ratio θa is equal to 120° inelectrical angle, it is impossible to utilize the harmonics of thethird-order group.

FIG. 20 shows the results of a computation using FEM (Finite ElementMethod) with the arc ratio θa set to 120° in electrical angle. In FIG.20, the fundamental wave (or the first-order harmonic) of the electriccurrent generated by the magnetic flux crossing the U-phase winding isindicated by a continuous line; the third-order harmonic of the electriccurrent is indicated by a dashed line with the amplitude of thethird-order harmonic magnified five times. As seen from FIG. 20, whenthe arc ratio θa is set to 120° in electrical angle, it is difficult toidentify the third-order harmonic even after magnifying the amplitude ofthe third-order harmonic five times in FIG. 20. Accordingly, it has beenmade clear that when the arc ratio θa is set to 120° in electricalangle, the third-order harmonic becomes almost zero.

On the other hand, when the arc ratio θa is not equal to 120° inelectrical angle, the rectangular waveform shown in FIG. 19 contains thewaveforms of the harmonics of the third-order group. To increase theq-axis inductance Lq, it is necessary to shift the phase of Am₃ sin 3ωt,which is the largest among the components constituting the harmonicelectric currents of the third-order group, from the first-ordercomponent by +60° in electrical angle. The condition for doing so isthat the arc ratio θa is less than 120° in electrical angle. However,after summing the magnetic fluxes respectively through the five unshadedteeth 33 of the stator core 31 in FIG. 14, the positive and negativesigns (or polarities) of the third-order harmonic of the electriccurrent are inverted within the range of 0° to 180° in electrical anglewith respect to the fundamental wave of the electric current (see FIGS.21-22). Consequently, the condition for increasing the q-axis inductanceLq becomes that the arc ratio θa is greater than 120° in electricalangle.

In addition, in FIG. 21, “INPUT” denotes the magnetic flux passingthrough one of the unshaded teeth 33 of the stator core 31 in FIG. 14;

“FUNDAMENTAL WAVE” denotes the fundamental wave (or the first-orderharmonic) of the electric current generated by the magnetic flux passingthrough the one unshaded tooth 33; and “3RD-ORDER HARMONIC” denotes thethird-order harmonic of the electric current generated by the magneticflux passing through the one unshaded tooth 33. On the other hand, inFIG. 22, “INPUT” denotes the sum of the magnetic fluxes respectivelythrough the five unshaded teeth 33 of the stator core 31 in FIG. 14(i.e., the magnetic flux crossing the U-phase winding); “FUNDAMENTALWAVE” denotes the fundamental wave (or the first-order harmonic) of theelectric current generated by the sum of the magnetic fluxes; and“3RD-ORDER HARMONIC” denotes the third-order harmonic of the electriccurrent generated by the sum of the magnetic fluxes.

Accordingly, in the present embodiment, the arc ratio θa of eachmagnetic pole of the rotor 20 is set to be greater than 120° inelectrical angle.

As shown in FIG. 23, in the present embodiment, the stator coil 35 isconfigured to be switchable between a Y connection and a Δ connection.

Specifically, in the present embodiment, the drive apparatus 50 includesa first inverter 54, a second inverter 55 and a three-phase full-waverectifier 56. Each of the U-phase, V-phase and W-phase windings of thestator coil 35 has first and second ends. The first ends of the U-phase,V-phase and W-phase windings are respectively connected to outputterminals u1, v1 and w1 of the first inverter 54. The second ends of theU-phase, V-phase and W-phase windings are respectively connected tooutput terminals u2, v2 and w2 of the second inverter 55. Moreover, thefirst ends of the U-phase, V-phase and W-phase windings are alsorespectively connected to input terminals R, S and T of the three-phasefull-wave rectifier 56 that is configured with six diodes D.

Each of the first and second inverters 54 and 55 is a three-phaseinverter of a well-known type. More specifically, the first inverter 54has a pair of DC terminals 54 a and 54 b respectively connected topositive and negative terminals of a vehicle battery (or DC powersource) B. Moreover, the first inverter 54 has one pair of switchingelements Tr per phase; the pair of switching elements Tr are connectedin series with each other between the DC terminals 54 a and 54 b. Thefirst inverter 54 inverts the DC output voltage of the vehicle battery Binto a three-phase AC voltage by controlling on/off operation of theswitching elements Tr. Similarly, the second inverter 55 has a pair ofDC terminals 55 a and 55 b respectively connected to the positive andnegative terminals of the vehicle battery B. Moreover, the secondinverter 55 has one pair of switching elements Tr per phase; the pair ofswitching elements Tr are connected in series with each other betweenthe DC terminals 55 a and 55 b. The second inverter 55 inverts the DCoutput voltage of the vehicle battery B into a three-phase AC voltage bycontrolling on/off operation of the switching elements Tr.

The three-phase full-wave rectifier 56 has a positive terminal 56 a, anegative terminal 56 b and a short-circuiting circuit 57 thatshort-circuits between the positive and negative terminals 56 a and 56b. The short-circuiting circuit 57 has an electronic switch 58 connectedbetween the positive and negative terminals 56 a and 56 b.

In addition, the operations of the first and second inverters 54 and 55and the on/off operation of the electronic switch 58 are controlled by anot-shown ECU (Electronic Control Unit) based on a signal outputted froma not-shown position sensor that senses the rotational position of therotor 20 of the rotating electric machine 1.

Next, operation of the rotating electric machine 1 will be described.

In the present embodiment, the rotating electric machine 1 operates ineither a Y connection mode or a Δ connection mode.

(a) Y Connection Mode

In driving the rotating electric machine 1 in a low-speed region, theelectronic switch 58 is turned on, thereby causing the second inverter55 to operate while keeping the first inverter 54 in an off state. Withthe electronic switch 58 being in an on state, the short-circuitingcircuit 57 short-circuits between the positive and negative terminals 56a and 56 b of the three-phase full-wave rectifier 56. Consequently, thefirst ends of the U-phase, V-phase and W-phase windings of the statorcoil 35 are connected to define a neutral point; the second ends of theU-phase, V-phase and W-phase windings are respectively connected to theoutput terminals u2, v2 and w2 of the second inverter 55. As a result,the stator coil 35 is Y-connected.

The ECU on/off controls the three pairs of switching elements Tr of thesecond inverter 55 in a manner of, for example, 180° energization with120° phase shift therebetween. Consequently, the three-phase AC voltageproduced by the second inverter 55 is applied to the Y-connected statorcoil 35. As a result, the rotating electric machine 1 functions as anelectric motor in which the total number of serially-connected electricconductors is equal to √3 M, where M is the number of serially-connectedelectric conductors per phase.

(b) Δ Connection Mode

In driving the rotating electric machine 1 in a high-speed region, theelectronic switch 58 is turned off, causing both the first and secondinverters 54 and 55 to operate in sync with each other. With theelectronic switch 58 being in an off state, the short-circuiting circuit57 is opened between the positive and negative terminals 56 a and 56 bof the three-phase full-wave rectifier 56. Consequently, the first endsof the U-phase, V-phase and W-phase windings of the stator coil 35 areno longer connected to define the neutral point; the circuitconfiguration of the stator coil 35 becomes equivalent to a Δconnection.

The ECU on/off controls the three pairs of switching elements Tr of thefirst inverter 54 as well as the three pairs of switching elements Tr ofthe second inverter 55 in a manner of, for example, 180° energizationwith 120° phase shift therebetween. Consequently, the three-phase ACvoltage produced by the first and second inverters 54 and 55 is appliedto the Δ-connected stator coil 35. As a result, the rotating electricmachine 1 functions as an electric motor in which the total number ofserially-connected electric conductors is equal to M.

Moreover, in the present embodiment, in the predetermined high-torqueregion where the magnet torque produced by the rotor 20 is lower thanthe reluctance torque produced by the rotor 20, the drive apparatus 50drives the rotating electric machine 1 to operate in the Δ connectionmode. Consequently, it is possible to increase the q-axis inductance Lq,thereby increasing the reluctance torque. As a result, it is possible toincrease the total torque produced by the rotor 20, thereby achieving ahigh efficiency of the rotating electric machine 1 in the predeterminedhigh-torque region as described in the first embodiment.

According to the present embodiment, it is possible to achieve thefollowing advantageous effects.

In the present embodiment, the rotating electric machine drive systemincludes the rotating electric machine 1 and the drive apparatus 50. Therotating electric machine 1 includes the stator 30 and the rotor 20. Thestator 30 includes the stator core 31 and the three-phase stator coil 35mounted on the stator core 31. The stator coil 35 is configured to beswitchable between the Y connection and the Δ connection. The rotor 20is configured to produce both the magnet torque and the reluctancetorque. The drive apparatus 50 supplies electric current to the statorcoil 35 and thereby drives the rotating electric machine 1. In thepredetermined high-torque region where the magnet torque produced by therotor 20 is lower than the reluctance torque produced by the rotor 20,the drive apparatus 50 supplies the electric current to the stator coil35 with the stator coil 35 switched to the Δ connection.

With the above configuration, in the predetermined high-torque region,it is possible to supply the Δ-connected stator coil 35 with theelectric current which has the waveform obtained by superimposing thespecific harmonic waveform on the first-order harmonic waveform.Consequently, it is possible to increase the q-axis inductance Lq,thereby increasing the reluctance torque. As a result, it is possible toincrease the total torque produced by the rotor 20, thereby achieving ahigh efficiency of the rotating electric machine 1 in the predeterminedhigh-torque region.

In the present embodiment, the arc ratio θa of each magnetic pole of therotor 20, which is the angular range within which magnetic flux radiallyflows from the pair of permanent magnets 23 forming the magnetic pole tothe stator 30, is set to be greater than 120° in electrical angle.

Setting the arc ratio θa as above, it is possible to create the specificharmonic waveform of the electric current supplied from the driveapparatus 50 to the stator coil 35. Consequently, it is possible toachieve a high efficiency of the rotating electric machine 1 in thepredetermined high-torque region, without controlling the electriccurrent as in the first embodiment.

[First Modification]

In the above-described third embodiment, each of the magnet-receivingholes 22 of the rotor core 21 is formed so that: the radially outer wallsurface of the magnet-receiving hole 22 abuts a radially outer sidesurface of the permanent magnet 23 received in the magnet-receiving hole22 over the entire length of the radially outer side surface of thepermanent magnet 23; and thus the extension wall surface 22 a extendingfrom the radially outer wall surface of the magnet-receiving hole 22does not face the radially outer side surface of the permanent magnet 23(see FIGS. 11 and 12).

In comparison, in this modification, as shown in FIGS. 24 and 25, eachof the magnet-receiving holes 22 of the rotor core 21 is formed so that:the radially outer wall surface of the magnet-receiving hole 22 abutsonly part of the radially outer side surface of the permanent magnet 23received in the magnet-receiving hole 22; and the extension wall surface22 a extending from the radially outer wall surface of themagnet-receiving hole 22 faces the radially outer side surface of thepermanent magnet 23 with a radial gap formed therebetween.

However, in this modification, the arc ratio θa of each magnetic pole ofthe rotor 20 can still be defined as described in the third embodiment.

Specifically, as shown in FIGS. 24 and 25, the arc ratio θa can bedefined as an angle between first and second imaginary lines L1 and L2.The first imaginary line L1 extends straight through both thelongitudinal axis O of the rotor core 21 and an intersection point P1;the intersection point P1 is formed between the extension wall surface22 a, which extends from the radially outer wall surface of themagnet-receiving hole 22 receiving one of the pair of permanent magnets23 (i.e., the left-side permanent magnet 23 in FIG. 24) toward the firstmagnetic flux barrier 25 adjacent to the magnet-receiving hole 22, andthe radially inner wall surface 28 a of the circumferentially-extendingbridge 28 which defines the first magnetic flux barrier 25. On the otherhand, the second imaginary line L2 extends straight through both thelongitudinal axis O of the rotor core 21 and an intersection point P2;the intersection point P2 is formed between the extension wall surface22 a, which extends from the radially outer wall surface of themagnet-receiving hole 22 receiving the other of the pair of permanentmagnets 23 (i.e., the right-side permanent magnet 23 in FIG. 24) towardthe first magnetic flux barrier 25 adjacent to the magnet-receiving hole22, and the radially inner wall surface 28 a of thecircumferentially-extending bridge 28 which defines the first magneticflux barrier 25.

[Second Modification]

In the above-described third embodiment, each magnetic pole of the rotor20 is formed of one pair of permanent magnets 23 arranged in thesubstantially V-shape that opens toward the radially outer periphery ofthe rotor core 21. Moreover, the rotor core 21 has a round radiallyouter surface without protrusions formed thereon (see FIG. 11).

In comparison, in this modification, as shown in FIG. 26, each magneticpole of the rotor 20 is formed of a single permanent magnet 23.Moreover, the rotor core 21 has a plurality of protrusions each of whichprotrudes radially outward from the radially outer surface of the rotorcore 21 and is radially aligned with the permanent magnet 23 forming oneof the magnetic poles of the rotor 20. Furthermore, each of theprotrusions has a radially outer surface 21 a and a pair of obliquesurfaces 21 b formed respectively on opposite circumferential ends ofthe radially outer surface 21 a as so to extend obliquely with respectto the radially outer surface 21 a.

In this modification, the arc ratio θa is defined as an angle betweenfirst and second imaginary lines L1 and L2. The first imaginary line L1extends straight through both the longitudinal axis O of the rotor core21 and an intersection point P1; the intersection point P1 is formedbetween the radially outer surface 21 a and one of the pair of obliquesurfaces 21 b (i.e., the left-side oblique surface 21 b in FIG. 26) ofthe protrusion. On the other hand, the second imaginary line L2 extendsstraight through both the longitudinal axis O of the rotor core 21 andan intersection point P2; the intersection point P2 is formed betweenthe radially outer surface 21 a and the other of the pair of obliquesurfaces 21 b (i.e., the right-side oblique surface 21 b in FIG. 26) ofthe protrusion.

[Third Modification]

As shown in FIG. 27, this modification differs from the above-describedsecond modification only in that each magnetic pole of the rotor 20 isformed of one pair of permanent magnets 23 arranged in a substantiallyV-shape that opens toward the radially outer periphery of the rotor core21.

In this modification, the arc ratio θa of each magnetic pole of therotor 20 can still be defined as described in the second modification.

Fourth Embodiment

A rotating electric machine drive system according to the fourthembodiment has a similar configuration to the rotating electric machinedrive system according to the third embodiment. Therefore, thedifferences therebetween will be mainly described hereinafter.

In the third embodiment, each of the teeth 33 of the stator core 31 hasno protrusions 33 a formed at a distal end thereof (see FIG. 11).Moreover, the arc ratio θa of each magnetic pole of the rotor 20 is setto be greater than 120° in electrical angle (i.e., θa>120°).

In comparison, in the present embodiment, as shown in FIG. 28, each ofthe teeth 33 of the stator core 31 has a pair of protrusions 33 a formedat a distal end (or radially inner end) thereof so as to protruderespectively toward opposite circumferential sides. Thus, as shown inFIG. 29, for each of the teeth 33 of the stator core 31, a distal endportion of the tooth 33 has a substantially T-shape. That is, with theprotrusions 33 a, the circumferential width of the distal end portion ofthe tooth 33 is increased.

Moreover, referring to FIG. 30, in the present embodiment, the followingrelationship is satisfied:

θx=θa+α≧120°,

where θx is an angular range in electrical angle within which the teeth33 of the stator core 31 receive magnetic flux from one magnetic pole ofthe rotor 20 and α is the circumferential width in electrical angle ofeach of the teeth 33 of the stator core 31 at the distal end thereof.

That is, in the present embodiment, the angular range θx within whichthe teeth 33 of the stator core 31 receive magnetic flux from onemagnetic pole of the rotor 20 is expanded to (θa+α) from θa in the thirdembodiment. Consequently, it is possible to collect and utilize magneticflux from each magnetic pole of the rotor 20 in a wider range.

Moreover, as shown in FIG. 30, magnetic flux emitted from one magneticpole of the rotor 20 and crossing the teeth 33 of the stator core 31 hasa substantially trapezoidal waveform. Consequently, with thesubstantially trapezoidal waveform of the magnetic flux, it is possibleto more easily create the desired harmonic electric currents of thethird-order group.

In terms of ease of controlling magnetic flux, it is preferable for theteeth 33 with the protrusions 33 a to have a short magnetic flux path.It is also preferable to cause the substantially T-shaped distal endportions of the teeth 33 to be magnetically saturated, thereby creatingthe desired harmonic electric currents of the third-order group. Inaddition, it is possible to cause the substantially T-shaped distal endportions of the teeth 33 to be magnetically saturated by forming thepermanent magnets 23 with a high Br material (e.g., neodymium, samariumor alnico) or replacing at least some of the permanent magnets 23 withelectromagnets

Moreover, to cause the substantially T-shaped distal end portions of theteeth 33 to be magnetically saturated, it is necessary to satisfy thefollowing relationship: Bd×Amag>Bs×Ast, where Bd is the magnetic fluxdensity of the magnets (permanent magnets 23 or electromagnets) in T,Amg is the area of the magnets in mm², Bs is the saturation flux densityof the stator 30 in T and Ast is the area of the stator 30 in mm².

In the case where the above relationship is not satisfied, it ispreferable to expand the angular range θx to (θa+α) as in the presentembodiment. In addition, the above relationship may not be satisfied inthe following cases: (1) the stator core 31 is formed of permendur; (2)the magnets are formed of a low Br material such as ferrite; (3) themagnets are electromagnets and exciting current supplied to theelectromagnets is low; and (4) though the material of the magnets has ahigh Br, the amount of the material used for forming the magnets issuppressed in the design of the magnets.

According to the present embodiment, it is possible to achieve the sameadvantageous effects as described in the third embodiment.

Moreover, in the present embodiment, since the angular range θx isexpanded to (θa+α), it is possible to more easily create the desiredharmonic electric currents of the third-order group.

Fifth Embodiment

A rotating electric machine drive system according to the fifthembodiment has a similar configuration to the rotating electric machinedrive system according to the fourth embodiment. Therefore, thedifferences therebetween will be mainly described hereinafter.

In the fourth embodiment, each magnetic pole of the rotor 20 is formedof one pair of permanent magnets 23 arranged in a substantially V-shapethat opens toward the radially outer periphery of the rotor core 21.Moreover, the relationship of θx=θa+α≧120° is satisfied (see FIGS.28-30).

In comparison, in the present embodiment, as shown in FIG. 31, eachmagnetic pole of the rotor 20 is formed of first and second magnets thatare arranged in the rotor core 21 to overlap each other in a radialdirection of the rotor core 21.

The first magnet is implemented by a pair of permanent magnets 23arranged in a substantially V-shape that opens toward the radially outerperiphery of the rotor core 21. Moreover, the pair of permanent magnets23 is symmetrically arranged with respect to the centerline C1 of themagnetic pole. However, the arc ratio θa of the first magnet (i.e., thepair of permanent magnets 23) is set to be less than 120° in electricalangle, unlike in the fourth embodiment. Here, the arc ratio θarepresents the angular range within which magnetic flux radially flowsfrom the first magnet to the stator 30.

The second magnet is implemented by a single permanent magnet 29. Thesecond magnet is arranged radially outside (i.e., on the stator 30 sideof) the first magnet and symmetrically with respect to the centerline C1of the magnetic pole. More specifically, the second magnet (i.e., thesingle permanent magnet 29) is received in a magnet-receiving hole 29Athat is formed in the rotor core 21 so as to be located radially outsidethe pair of magnet-receiving holes 22 receiving the pair of permanentmagnets 23 and symmetrical with respect to the centerline C1 of themagnetic pole. Moreover, the arc ratio θb of the second magnet is set tobe less than the arc ratio θa of the first magnet. Here, the arc ratioθb represents the angular range within which magnetic flux radiallyflows from the second magnet to the stator 30.

In the present embodiment, since the first and second magnets arearranged in the rotor core 21 to overlap each other in the radialdirection, the phases of the harmonics of the third-order group areinverted within the range where the arc ratio θa of the first magnet(i.e., the pair of permanent magnets 23) and the arc ratio θb of thesecond magnet (i.e., the single permanent magnet 29) overlap.Consequently, even with the arc ratio θa of the first magnet set to beless than 120° in electrical angle, it is still possible to create thespecific harmonic waveform described in the first embodiment, therebyachieving a high efficiency of the rotating electric machine 1.

In addition, it should be noted that the second magnet may also beimplemented by a pair of permanent magnets which are arranged in asubstantially V-shape that opens toward the radially outer periphery ofthe rotor core 21.

Comparative Example

In this example, as shown in FIG. 32, the second magnet (i.e., thesingle permanent magnet 29) is arranged radially inside (i.e., on thenon-stator 30 side of) the first magnet (i.e., the pair of permanentmagnets 23).

With the above arrangement, the phase inversion described in the fifthembodiment does not occur even if the arc ratio θa of the first magnetis set to be less than 120° in electrical angle and the arc ratio θb ofthe second magnet is set to be less than the arc ratio θa of the firstmagnet. Consequently, it is impossible to create the specific harmonicwaveform.

Other Embodiments

While the above particular embodiments have been shown and described, itwill be understood by those skilled in the art that the presentinvention can also be embodied in various other modes without departingfrom the spirit of the present invention.

For example, in the above-described embodiments, the present inventionis directed to a drive system for the rotating electric machine 1 thatis configured as an electric motor for use in a motor vehicle. However,the present invention can also be applied to drive systems for otherrotating electric machines, such as a drive system for an electricgenerator or a drive system for a motor-generator that selectivelyfunctions either as an electric motor or as an electric generator.

Moreover, in the above-described embodiments, the present invention isdirected to a drive system for the rotating electric machine 1 that isof an inner rotor type. However, the present invention can also beapplied to a drive system for an outer rotor-type rotating electricmachine.

What is claimed is:
 1. A rotating electric machine drive systemcomprising: a rotating electric machine including a Y-connectedthree-phase stator coil and a rotor that produces both magnet torque andreluctance torque; and a drive apparatus that supplies electric currentto the stator coil and thereby drives the rotating electric machine,wherein in a predetermined high-torque region, the drive apparatussupplies the stator coil with the electric current which has a waveformobtained by superimposing a specific harmonic waveform on a first-orderharmonic waveform, the specific harmonic waveform being one ofthird-order and (3+6n)th-order harmonic waveforms, or a harmonicwaveform which is obtained by synthesizing at least two of thethird-order and (3+6n)th-order harmonic waveforms, where n is a naturalnumber greater than or equal to 1, the specific harmonic waveform takinga negative integral value for a positive half cycle of the first-orderharmonic waveform and a positive integral value for a negative halfcycle of the first-order harmonic waveform.
 2. The rotating electricmachine drive system as set forth in claim 1, wherein the high-torqueregion is predetermined as an operating region of the rotating electricmachine where the magnet torque produced by the rotor is lower than thereluctance torque produced by the rotor.
 3. The rotating electricmachine drive system as set forth in claim 1, wherein the high-torqueregion is predetermined so that in the high-torque region, the followingequation is satisfied:T=pΨIq+p(Lq−Ld)IdIq where T is the total torque produced by the rotor, pis the number of magnetic pole pairs of the rotor, Ψ is magnet magneticflux, Iq is q-axis electric current, Id is d-axis electric current, Lqis q-axis inductance and Ld is d-axis inductance.
 4. A rotating electricmachine drive system comprising: a rotating electric machine including astator and a rotor, the stator including a stator core and a three-phasestator coil mounted on the stator core, the rotor being configured toproduce both magnet torque and reluctance torque; and a drive apparatusthat supplies electric current to the stator coil and thereby drives therotating electric machine, wherein the stator coil is Δ-connected, andin a predetermined high-torque region where the magnet torque producedby the rotor is lower than the reluctance torque produced by the rotor,the drive apparatus performs one of a PWM control with a PWM frequencybeing not higher than an audible range and an overmodulation control. 5.The rotating electric machine drive system as set forth in claim 4,wherein the high-torque region is predetermined so that in thehigh-torque region, the following equation is satisfied:T=pΨIq+p(Lq−Ld)IdIq where T is the total torque produced by the rotor, pis the number of magnetic pole pairs of the rotor, Ψ is magnet magneticflux, Iq is q-axis electric current, Id is d-axis electric current, Lqis q-axis inductance and Ld is d-axis inductance.
 6. The rotatingelectric machine drive system as set forth in claim 4, wherein the rotorincludes a rotor core disposed in radial opposition to the stator coreand a plurality of magnets provided in the rotor core, the magnetsforming a plurality of magnetic poles on a stator-side periphery of therotor core so that polarities of the magnetic poles alternate between Nand S in a circumferential direction of the rotor core, and an arc ratioθa of each magnetic pole of the rotor, which is an angular range withinwhich magnetic flux radially flows from the magnetic pole to the stator,is set to be greater than 120° in electrical angle, so as to create aspecific harmonic waveform of the electric current supplied from thedrive apparatus to the stator coil, the specific harmonic waveform beingone of third-order and (3+6n)th-order harmonic waveforms, or a harmonicwaveform which is obtained by synthesizing at least two of thethird-order and (3+6n)th-order harmonic waveforms, where n is a naturalnumber greater than or equal to 1, the specific harmonic waveform takinga negative integral value for a positive half cycle of a first-orderharmonic waveform of the electric current and a positive integral valuefor a negative half cycle of the first-order harmonic waveform.
 7. Therotating electric machine drive system as set forth in claim 4, whereinthe rotor includes a rotor core disposed in radial opposition to thestator core and a plurality of magnets provided in the rotor core, themagnets forming a plurality of magnetic poles on a stator-side peripheryof the rotor core so that polarities of the magnetic poles alternatebetween N and S in a circumferential direction of the rotor core, thestator core has a plurality of teeth each radially extending toward therotor and being spaced from one another at a predetermined pitch in acircumferential direction of the stator core, each of the teeth of thestator core has a pair of protrusions formed at a distal end thereof soas to protrude respectively toward opposite circumferential sides, andthe following relationship is satisfied: θx=θa+α≧120°, where θx is anangular range in electrical angle within which the teeth of the statorcore receives magnetic flux from one magnetic pole of the rotor, θa isan arc ratio of each magnetic pole of the rotor, the arc ratio being anangular range in electrical angle within which magnetic flux radiallyflows from the magnetic pole to the stator, and a is a circumferentialwidth in electrical angle of each of the teeth of the stator core at thedistal end thereof.
 8. The rotating electric machine drive system as setforth in claim 4, wherein the rotor includes a rotor core disposed inradial opposition to the stator core and a plurality of magnetic polesformed on a stator-side periphery of the rotor core so that polaritiesof the magnetic poles alternate between N and S in a circumferentialdirection of the rotor core, each of the magnetic poles of the rotor isformed of first and second magnets that are arranged in the rotor coreto overlap each other in a radial direction of the rotor core, an arcratio θa of the first magnet, which is an angular range within whichmagnetic flux radially flows from the first magnet to the stator, is setto be less than 120° in electrical angle, and the second magnet isarranged on the stator side of the first magnet, and an arc ratio θb ofthe second magnet, which is an angular range within which magnetic fluxradially flows from the second magnet to the stator, is set to be lessthan the arc ratio θa of the first magnet.
 9. A rotating electricmachine drive system comprising: a rotating electric machine including astator and a rotor, the stator including a stator core and a three-phasestator coil mounted on the stator core, the rotor being configured toproduce both magnet torque and reluctance torque; and a drive apparatusthat supplies electric current to the stator coil and thereby drives therotating electric machine, wherein the stator coil is configured to beswitchable between a Y connection and a Δ connection, and in apredetermined high-torque region where the magnet torque produced by therotor is lower than the reluctance torque produced by the rotor, thedrive apparatus supplies the electric current to the stator coil withthe stator coil switched to the Δ connection.
 10. The rotating electricmachine drive system as set forth in claim 9, wherein the high-torqueregion is predetermined so that in the high-torque region, the followingequation is satisfied:T=pΨIq+p(Lq−Ld)IdIq where T is the total torque produced by the rotor, pis the number of magnetic pole pairs of the rotor, Ψ is magnet magneticflux, Iq is q-axis electric current, Id is d-axis electric current, Lqis q-axis inductance and Ld is d-axis inductance.
 11. The rotatingelectric machine drive system as set forth in claim 9, wherein the rotorincludes a rotor core disposed in radial opposition to the stator coreand a plurality of magnets provided in the rotor core, the magnetsforming a plurality of magnetic poles on a stator-side periphery of therotor core so that polarities of the magnetic poles alternate between Nand S in a circumferential direction of the rotor core, and an arc ratioθa of each magnetic pole of the rotor, which is an angular range withinwhich magnetic flux radially flows from the magnetic pole to the stator,is set to be greater than 120° in electrical angle, so as to create aspecific harmonic waveform of the electric current supplied from thedrive apparatus to the stator coil, the specific harmonic waveform beingone of third-order and (3+6n)th-order harmonic waveforms, or a harmonicwaveform which is obtained by synthesizing at least two of thethird-order and (3+6n)th-order harmonic waveforms, where n is a naturalnumber greater than or equal to 1, the specific harmonic waveform takinga negative integral value for a positive half cycle of a first-orderharmonic waveform of the electric current and a positive integral valuefor a negative half cycle of the first-order harmonic waveform.
 12. Therotating electric machine drive system as set forth in claim 9, whereinthe rotor includes a rotor core disposed in radial opposition to thestator core and a plurality of magnets provided in the rotor core, themagnets forming a plurality of magnetic poles on a stator-side peripheryof the rotor core so that polarities of the magnetic poles alternatebetween N and S in a circumferential direction of the rotor core, thestator core has a plurality of teeth each radially extending toward therotor and being spaced from one another at a predetermined pitch in acircumferential direction of the stator core, each of the teeth of thestator core has a pair of protrusions formed at a distal end thereof soas to protrude respectively toward opposite circumferential sides, andthe following relationship is satisfied: θx=θa+α≧120°, where θx is anangular range in electrical angle within which the teeth of the statorcore receives magnetic flux from one magnetic pole of the rotor, θa isan arc ratio of each magnetic pole of the rotor, the arc ratio being anangular range in electrical angle within which magnetic flux radiallyflows from the magnetic pole to the stator, and a is a circumferentialwidth in electrical angle of each of the teeth of the stator core at thedistal end thereof.
 13. The rotating electric machine drive system asset forth in claim 9, wherein the rotor includes a rotor core disposedin radial opposition to the stator core and a plurality of magneticpoles formed on a stator-side periphery of the rotor core so thatpolarities of the magnetic poles alternate between N and S in acircumferential direction of the rotor core, each of the magnetic polesof the rotor is formed of first and second magnets that are arranged inthe rotor core to overlap each other in a radial direction of the rotorcore, an arc ratio θa of the first magnet, which is an angular rangewithin which magnetic flux radially flows from the first magnet to thestator, is set to be less than 120° in electrical angle, and the secondmagnet is arranged on the stator side of the first magnet, and an arcratio θb of the second magnet, which is an angular range within whichmagnetic flux radially flows from the second magnet to the stator, isset to be less than the arc ratio θa of the first magnet.